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Mechanics () is the area of concerned with the relationships between , , and among .

(2026). 9781292314730, Pearson Education.
Forces applied to objects may result in displacements, which are changes of an object's position relative to its environment.

Theoretical expositions of this branch of have their origins in , for instance, in the writings of and Dugas, Rene. A History of Classical Mechanics. New York, NY: Dover Publications Inc, 1988, pg 19.Rana, N.C., and Joag, P.S. Classical Mechanics. West Petal Nagar, New Delhi. Tata McGraw-Hill, 1991, pg 6.Renn, J., Damerow, P., and McLaughlin, P. Aristotle, Archimedes, Euclid, and the Origin of Mechanics: The Perspective of Historical Epistemology. Berlin: Max Planck Institute for the History of Science, 2010, pg 1-2. (see History of classical mechanics and Timeline of classical mechanics). During the early modern period, scientists such as , , Christiaan Huygens, and laid the foundation for what is now known as classical mechanics.

In the 20th century the concepts of classical mechanics were challenged by new discoveries, leading to fundamentally new approaches including relativistic mechanics and quantum mechanics.


History

Antiquity
The ancient were among the first to propose that abstract principles govern nature. The main theory of mechanics in antiquity was Aristotelian mechanics, though an alternative theory is exposed in the Mechanical Problems, often attributed to one of his successors.

There is another tradition that goes back to the ancient Greeks where mathematics is used more extensively to analyze bodies or dynamically, an approach that may have been stimulated by prior work of the Pythagorean .

(2026). 9780199289318, OUP Oxford. .
Examples of this tradition include pseudo- ( On the Balance), ( On the Equilibrium of Planes, On Floating Bodies), Hero ( Mechanica), and Pappus ( Collection, Book VIII)." A history of mechanics". René Dugas (1988). p.19. " A Tiny Taste of the History of Mechanics". The University of Texas at Austin.


Medieval age
In the Middle Ages, Aristotle's theories were criticized and modified by a number of figures, beginning with in the 6th century. A central problem was that of projectile motion, which was discussed by and Philoponus.

Persian Islamic polymath Ibn Sīnā published his theory of motion in The Book of Healing (1020). He said that an impetus is imparted to a projectile by the thrower, and viewed it as persistent, requiring external forces such as to dissipate it.

(1996). 9780700703142, .
Ibn Sina made a distinction between 'force' and 'inclination' (called "mayl"), and argued that an object gained mayl when the object is in opposition to its natural motion. So he concluded that continuation of motion is attributed to the inclination that is transferred to the object, and that object will be in motion until the mayl is spent. He also claimed that a projectile in a vacuum would not stop unless it is acted upon, consistent with Newton's first law of motion.

On the question of a body subject to a constant (uniform) force, the 12th-century Jewish-Arab scholar Hibat Allah Abu'l-Barakat al-Baghdaadi (born Nathanel, Iraqi, of Baghdad) stated that constant force imparts constant acceleration. According to , al-Baghdaadi's theory of motion was "the oldest negation of 's fundamental dynamic law namely,, and anticipation in a vague fashion of the fundamental law of classical mechanics namely,."
(cf. Abel B. Franco (October 2003). "Avempace, Projectile Motion, and Impetus Theory", Journal of the History of Ideas 64 (4), p. 521-546 528.)

Influenced by earlier writers such as Ibn Sina and al-Baghdaadi, the 14th-century French priest developed the theory of impetus, which later developed into the modern theories of , , and . This work and others were developed in 14th-century England by the Oxford Calculators such as Thomas Bradwardine, who studied and formulated various laws regarding falling bodies. The concept that the main properties of a body are uniformly accelerated motion (as of falling bodies) was worked out by the 14th-century Oxford Calculators.


Early modern age
Two central figures in the early modern age are and . Galileo's final statement of his mechanics, particularly of falling bodies, is his Two New Sciences (1638). Newton's 1687 Philosophiæ Naturalis Principia Mathematica provided a detailed mathematical account of mechanics, using the newly developed mathematics of and providing the basis of Newtonian mechanics.

There is some dispute over the priority of various ideas: Newton's Principia is certainly the seminal work and has been tremendously influential, and many of the mathematical results therein could not have been stated earlier without the development of the calculus. However, many of the ideas, particularly as they pertain to inertia and falling bodies, had been developed by prior scholars such as Christiaan Huygens and the less-known medieval predecessors. Assigning precise credit is difficult, since scientific language and standards of proof have changed; the ideas of medieval scholars may be regarded either as equivalent to modern statements or merely as preliminary hypotheses similar to them.


Modern age
Two main modern developments in mechanics are general relativity of , and quantum mechanics, both developed in the 20th century based in part on earlier 19th-century ideas. The development in the modern continuum mechanics, particularly in the areas of elasticity, plasticity, fluid dynamics, electrodynamics, and thermodynamics of deformable media, started in the second half of the 20th century.


Types of mechanical bodies
The often-used term needs to stand for a wide assortment of objects, including , , , , parts of machinery, parts of , parts of ( and ), etc.

Other distinctions between the various sub-disciplines of mechanics concern the nature of the bodies being described. Particles are bodies with little (known) internal structure, treated as mathematical points in classical mechanics. Rigid bodies have size and shape, but retain a simplicity close to that of the particle, adding just a few so-called degrees of freedom, such as orientation in space.

Otherwise, bodies may be semi-rigid, i.e. elastic, or non-rigid, i.e. . These subjects have both classical and quantum divisions of study.

For instance, the motion of a spacecraft, regarding its and attitude (), is described by the relativistic theory of classical mechanics, while the analogous movements of an are described by quantum mechanics.


Sub-disciplines
The following are the three main designations consisting of various subjects that are studied in mechanics.

Note that there is also the "theory of fields" which constitutes a separate discipline in physics, formally treated as distinct from mechanics, whether it be classical fields or quantum fields. But in actual practice, subjects belonging to mechanics and fields are closely interwoven. Thus, for instance, forces that act on particles are frequently derived from fields ( or ), and particles generate fields by acting as sources. In fact, in quantum mechanics, particles themselves are fields, as described theoretically by the .


Classical
explains Newton's law of gravitation in course 8.01 ]] The following are described as forming classical mechanics:
  • Newtonian mechanics: the original theory of motion () and forces (dynamics)
  • Analytical mechanics is a reformulation of Newtonian mechanics with an emphasis on system energy, rather than on forces. There are two main branches of analytical mechanics:
    • Hamiltonian mechanics: a theoretical formalism, based on the principle of conservation of energy
    • Lagrangian mechanics: another theoretical formalism, based on the principle of the
  • Classical statistical mechanics generalizes ordinary classical mechanics to consider systems in an unknown state; often used to derive properties.
  • Celestial mechanics: the motion of bodies in space: planets, comets, stars, , etc.
  • : spacecraft , etc.
  • : elasticity, plasticity, or exhibited by deformable solids
  • Fracture mechanics
  • : (density, variation, propagation) in solids, fluids and gases
  • : semi-rigid bodies in mechanical equilibrium
  • : the motion of fluids
  • : mechanical behavior of soils
  • Continuum mechanics: mechanics of continua (both solid and fluid)
  • : mechanical properties of liquids
  • : liquids in equilibrium
  • Applied mechanics (also known as engineering mechanics)
  • : solids, fluids, etc. in biology
  • : physical processes in living organisms
  • Relativistic or mechanics


Quantum
The following are categorized as being part of quantum mechanics:
  • Schrödinger wave mechanics: used to describe the movements of the wavefunction of a single particle.
  • is an alternative formulation that allows considering systems with a finite-dimensional state space.
  • Quantum statistical mechanics generalizes ordinary quantum mechanics to consider systems in an unknown state; often used to derive properties.
  • : the motion, structure, and behavior of fundamental particles
  • : the motion, structure, and reactions of nuclei
  • Condensed matter physics: quantum gases, solids, liquids, etc.

Historically, classical mechanics had been around for nearly a quarter millennium before quantum mechanics developed. Classical mechanics originated with 's laws of motion in Philosophiæ Naturalis Principia Mathematica, developed over the seventeenth century. Quantum mechanics developed later, over the nineteenth century, precipitated by and Albert Einstein's explanation of the photoelectric effect. Both fields are commonly held to constitute the most certain knowledge that exists about physical nature.

Classical mechanics has especially often been viewed as a model for other so-called . Essential in this respect is the extensive use of in theories, as well as the decisive role played by in generating and testing them.

Quantum mechanics is of a bigger scope, as it encompasses classical mechanics as a sub-discipline which applies under certain restricted circumstances. According to the correspondence principle, there is no contradiction or conflict between the two subjects, each simply pertains to specific situations. The correspondence principle states that the behavior of systems described by quantum theories reproduces classical physics in the limit of large , i.e. if quantum mechanics is applied to large systems (for e.g. a baseball), the result would almost be the same if classical mechanics had been applied. Quantum mechanics has superseded classical mechanics at the foundation level and is indispensable for the explanation and prediction of processes at the molecular, atomic, and sub-atomic level. However, for macroscopic processes classical mechanics is able to solve problems which are unmanageably difficult (mainly due to computational limits) in quantum mechanics and hence remains useful and well used. Modern descriptions of such behavior begin with a careful definition of such quantities as displacement (distance moved), time, velocity, acceleration, mass, and force. Until about 400 years ago, however, motion was explained from a very different point of view. For example, following the ideas of Greek philosopher and scientist Aristotle, scientists reasoned that a cannonball falls down because its natural position is in the Earth; the Sun, the Moon, and the stars travel in circles around the Earth because it is the nature of heavenly objects to travel in perfect circles.

Often cited as father to modern science, brought together the ideas of other great thinkers of his time and began to calculate motion in terms of distance travelled from some starting position and the time that it took. He showed that the speed of falling objects increases steadily during the time of their fall. This acceleration is the same for heavy objects as for light ones, provided air friction (air resistance) is discounted. The English mathematician and physicist improved this analysis by defining force and mass and relating these to acceleration. For objects traveling at speeds close to the speed of light, Newton's laws were superseded by 's theory of relativity. A For atomic and subatomic particles, Newton's laws were superseded by quantum theory. For everyday phenomena, however, Newton's three laws of motion remain the cornerstone of dynamics, which is the study of what causes motion.


Relativistic
Akin to the distinction between quantum and classical mechanics, 's general and special theories of relativity have expanded the scope of and 's formulation of mechanics. The differences between relativistic and Newtonian mechanics become significant and even dominant as the velocity of a body approaches the speed of light. For instance, in Newtonian mechanics, the of a is , whereas in relativistic mechanics, it is (where is the ; this formula reduces to the Newtonian expression in the low energy limit).

For high-energy processes, quantum mechanics must be adjusted to account for special relativity; this has led to the development of quantum field theory.

(2005). 9780521670531, Cambridge University Press.


Professional organizations
  • Applied Mechanics Division, American Society of Mechanical Engineers
  • Fluid Dynamics Division, American Physical Society
  • Society for Experimental Mechanics
  • International Union of Theoretical and Applied Mechanics


See also
  • Action principles
  • Applied mechanics
  • Computational mechanics
  • Mechanical engineering
  • Index of engineering science and mechanics articles
  • Kinetics
  • Non-autonomous mechanics
  • Wiesen Test of Mechanical Aptitude (WTMA)


Further reading


External links

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